Physics Letters B (Aug 2024)

Suppressed electric quadrupole collectivity in 49Ti

  • T.J. Gray,
  • J.M. Allmond,
  • C. Benetti,
  • C. Wibisono,
  • L. Baby,
  • A. Gargano,
  • T. Miyagi,
  • A.O. Macchiavelli,
  • A.E. Stuchbery,
  • J.L. Wood,
  • S. Ajayi,
  • J. Aragon,
  • B.W. Asher,
  • P. Barber,
  • S. Bhattacharya,
  • R. Boisseau,
  • J.M. Christie,
  • A.L. Conley,
  • P. De Rosa,
  • D.T. Dowling,
  • C. Esparza,
  • J. Gibbons,
  • K. Hanselman,
  • J.D. Holt,
  • S. Lopez-Caceres,
  • E. Lopez Saavedra,
  • G.W. McCann,
  • A. Morelock,
  • B. Kelly,
  • T.T. King,
  • B.C. Rasco,
  • V. Sitaraman,
  • S.L. Tabor,
  • E. Temanson,
  • V. Tripathi,
  • I. Wiedenhöver,
  • R.B. Yadav

Journal volume & issue
Vol. 855
p. 138856

Abstract

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Single-step Coulomb excitation of 46,48,49,50Ti is presented. A complete set of E2 matrix elements for the quintuplet of states in 49Ti, centred on the 2+ core excitation, was measured for the first time. A total of nine E2 matrix elements are reported, four of which were previously unknown. 2249Ti27 shows a 20% quenching in electric quadrupole transition strength as compared to its semi-magic 2250Ti28 neighbour. This 20% quenching, while empirically unprecedented, can be explained with a remarkably simple two-state mixing model, which is also consistent with other ground-state properties such as the magnetic dipole moment and electric quadrupole moment. A connection to nucleon transfer data and the quenching of single-particle strength is also demonstrated. The simplicity of the 49Ti-50Ti pair (i.e., approximate single-j 0f7/2 valence space and isolation of yrast states from non-yrast states) provides a unique opportunity to disentangle otherwise competing effects in the ground-state properties of atomic nuclei, the emergence of collectivity, and the role of proton-neutron interactions.